GB2199418A - Branching optical fibre coupler having biochemical tapers - Google Patents
Branching optical fibre coupler having biochemical tapers Download PDFInfo
- Publication number
- GB2199418A GB2199418A GB08706678A GB8706678A GB2199418A GB 2199418 A GB2199418 A GB 2199418A GB 08706678 A GB08706678 A GB 08706678A GB 8706678 A GB8706678 A GB 8706678A GB 2199418 A GB2199418 A GB 2199418A
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- fibres
- fibre
- coupler
- couplers
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- 239000013307 optical fiber Substances 0.000 title description 2
- 239000000835 fiber Substances 0.000 claims abstract description 45
- 230000003287 optical effect Effects 0.000 claims abstract description 22
- 238000000034 method Methods 0.000 claims description 25
- 238000004519 manufacturing process Methods 0.000 claims description 14
- 230000008569 process Effects 0.000 claims description 14
- 238000004382 potting Methods 0.000 claims description 2
- 150000001875 compounds Chemical class 0.000 claims 1
- 230000008878 coupling Effects 0.000 description 8
- 238000010168 coupling process Methods 0.000 description 8
- 238000005859 coupling reaction Methods 0.000 description 8
- 230000004044 response Effects 0.000 description 8
- 230000003595 spectral effect Effects 0.000 description 7
- 230000008901 benefit Effects 0.000 description 3
- 238000010438 heat treatment Methods 0.000 description 3
- 238000012544 monitoring process Methods 0.000 description 3
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 2
- 230000009471 action Effects 0.000 description 2
- 239000011248 coating agent Substances 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 239000000523 sample Substances 0.000 description 2
- 230000008859 change Effects 0.000 description 1
- 238000005253 cladding Methods 0.000 description 1
- 230000001427 coherent effect Effects 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000010355 oscillation Effects 0.000 description 1
- 238000011896 sensitive detection Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 239000000377 silicon dioxide Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29331—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by evanescent wave coupling
- G02B6/29332—Wavelength selective couplers, i.e. based on evanescent coupling between light guides, e.g. fused fibre couplers with transverse coupling between fibres having different propagation constant wavelength dependency
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/268—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light using optical fibres
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/2804—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers
- G02B6/2821—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers using lateral coupling between contiguous fibres to split or combine optical signals
- G02B6/2835—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers using lateral coupling between contiguous fibres to split or combine optical signals formed or shaped by thermal treatment, e.g. couplers
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/2804—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers
- G02B6/2856—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals forming multipart couplers without wavelength selective elements, e.g. "T" couplers, star couplers formed or shaped by thermal heating means, e.g. splitting, branching and/or combining elements
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Light Guides In General And Applications Therefor (AREA)
Abstract
An NxN optical coupler where N is at least equal to 4 is made by locating two pairs of optical fibres 1, 2, 4, 5 side by side, applying simultaneous tension and heat to the fibres so as to generate a biconical taper in the fibres so located, and to cause the fibres of each pair to fuse together to form two couplers. displacing one fibre of each pair so that each displaced fibre lies in the position vacated by the other fibre, and generating a second biconical taper in the rearranged fibres so as to fabricate two further couplers. <IMAGE>
Description
Optical Couplers
The present invention concerns fibre optic couplers.
It is well known to fabricate fibre optical couplers by a process which involves stripping the primary coating from a short length of a fibre optic, clamping the fibre in a motorised pulling arrangement so that the stripped portion can be stretched, and then heating the stripped portion whilst stretching the fibre. This action results in a bi-conical taper and by launching light of a specified wavelength from one end of the fibre and monitoring the light emitted at the other end a coupler can be produced the characteristics of which are dependent on the degree of the treatment. The basic principles involved in fabricating fibre optic couplers of this kind are disclosed in our copending U.K. Patent Application
No. 8519086, the contents of which are hereby incorporated in the present specification.
Problems arise when it is wished to fabricate single mode optic couplers of this type which have four or more input ports and four or more output ports.
In particular it can be shown that the maximum number n of fibres which can be fused together to produce 7xn equal power splitter is 3, giving a 3x3 coupler.
To fabricate couplers which have more than 3x3 inputs and outputs it is possible to cascade a number of 2x2 or 3x3 couplers. This, however, is very tedious, time consuming and expensive. The resultant coupler cannot be accomodated in a small space.
The present invention has for an object to provide a method of fabricating fibre-optic couplers of the type having at least 4 input and at least 4 output ports which is simpler than the above described process.
Accordingly from one aspect the present invention consists in a method of fabricating an NxN optical coupler where N is at least equal to 4, the method comprising the steps of locating two pairs of monomode optical fibres side by side, applying simultaneous tension and heat to the fibres so as to generate a biconical taper in the fibres so located and to cause the fibres of each pair to fuse together to form two couplers, displacing one fibre of each pair so that each displaced fibre lies in the position vacated by the other fibre, and generating a second biconical taper in the rearranged fibres so as to fabricate two further couplers.
The invention also consists in an optical coupler fabricated as aforesaid, and in an optical instrument such as an optical gyroscope incorporating such an optical coupler.
A still further application of the invention lies in the fabrication of N channel multiplexer/demultiplexers.
In order that the present invention may be more readily understood, an embodiment thereof will now be described by way of example and with reference to the accompanying drawings,in which:
Figure 1 is a diagrammatic view of a single mode 4x4 optic coupler,
Figure 2 is a diagrammatic plan view showing an early stage in the fabrication of a 4x4 optic coupler,
Figure 3a, b and c show successive stages in the fabrication of a 4x4 optic coupler,
Figure 4 is a diagram of a fibre optic gyroscope incorporating a 4x4 optic coupler,
Figure 5 is a diagrammatic view of a 4 channel demultiplexer,
Figure 6 is a graph showing spectral responses,
Figure 7 is a more detailed view, and two cross sections of the multiplexer of Figure 5,
Figure 8 shows three steps in manufacturing a 4x4 coupler fabricated without the use of a dummy fibre,
Figure 9 shows such a 4x4 coupler,
Figure 10 shows an optical sensor manufactured using the techniques of Figures 8 and 9,
Figure 11 shows how the sensor of Figure 10 can be manufactured, and
Figure 12 is a view of the fibres making up the sensor of Figure 10.
Referring now to the accompanying drawings the optical coupler shown in Figure 1 has four input ports a, b, c and d, respectively coupled by monomode optical fibres to form output ports a', b', c' and d'. This coupler is fabricated in the following manner. Five fibres 1 to 5 are stripped of their primary coating for a length of about 90mm. The fibres are placed side by side as is shown in the plan view of Figure 2 and are held by a pair of clamps 6 and 7, the clamps being formed with respective grooves 8 and 9 in which the fibres lie. The outer fibres 1, 2, 3 and 4 are all 8y-m/125un monomode optical waveguides whilst fibre 5 is a 125m diameter silica rod.
The area marked 10 is then heated with an oxybutane torch and the motorised clamps 6 and 7 driven away from one another so that the clamped portion is simultaneously heated and stretched. Whilst this is done optical power at a selected wavelength is injected into the left-hand ends of fibres 1 and 5 and monitored by suitable known detection equipment at the other, right-hand, ends of fibres 1, 2, 4 and 5. When the outputs of the four monitored fibres are identical the motorised pulling stages are stopped and the heat removed. The result of this operation is shown in
Figure 3a and consists of two couplers in parallel. As will now be appreciated the fibre 3 is a dummy fibre which serves as extra cladding material between the two parallel couplers and also serves to isolate them electro-mechanically.
The next step in the fabrication of a 4x4 coupler is shown in Figure 3b. Fibres 2 and 4 are crossed over dummy fibre 3 so that the numbering sequence of the fibres changes from 1, 2, 3, 4, 5 to 1, 4, 3, 2, 5. The new arrangement is then reclamped in the clamps 6 and 7 of the motorised pulling arrangement. If at this time light is launched down fibre 1 the outputs of fibres 1 and 2 would read the same power whilst the outputs of fibres 4 and 5 would read zero power.
The heating and stretching process is begun and during the process optical power is injected only into fibre 1 whilst the outputs of fibres 1, 2, 4 and 5 are simultaneously monitored. In this case the tapering process is stopped when all the fibre outputs read identically. The result is that two further couplers have been created which are again isolated from one another by the dummy fibre. Light launched down any one of the four input ports is distributed amongst the free output ports.
A 4x4 coupler has many potential applications.
One such application is in the manufacture of an optically modulated fibre-optic gyroscope. Such a gyroscope is shown diagrammatically in Figure 4.
In the gyroscope of Figure 4 light is launched via input 50 and is split into two at the first coupler 51.
The light is then directed into an N-turn fibre-optic coil 52 so that two coherent beams travel around coil 52 in opposite directions. The two initial beams from coupler 51 are indicated by arrows A. The beams emerge from the coil 52 and are respectively split by couplers 53, 54 and via coupler sections 51 and 55 emerge from the outputs 56, 57 and 58. Input 50 does not function both as an input and as an output. Outputs 56 and 57 are secondary outputs where the path difference between the lengths of coupler 54 to coupler 55 and coupler 53 to coupler 55 determine how the device is biased.
Ir
For sensitive detection a path difference of is required. It is another advantage of the coupler structure according to the present invention that such a path difference can be achieved with relative ease.
It can be seen from Figure 3e that if the portion where the fibres 2 and 4 are crossed over the dummy fibre is stretched there will be a differential change between the path lengths of the straight fibres 1 and 5 and the angled fibres 2 and 4. Thus by imparting a small extension to the cross-over portion and monitoring the angle of light through the couplers the desired path difference can readily be achieved.
Whilst the foregoing description has been limited to a 4x4 coupler it will-be appreciated that the use of one or more dummy fibres can be used in the fabrication of couplers having a greater number of inputs and outputs.
It will be appreciated that there are many other potential applications for nxn couplers where n is at least 4.
Couplers in which n is greater than 4 can be made in a manner analogous to that used to fabricate the 4x4 coupler.
Thus an NxN coupler can be fabricated using two or more dummy fibres. In each case the dummy fibre would provide separation between a pair of couplers formed as before by tapering, with each pair of separated couplers being linked by the process of moving the two active fibres adjacent the (each of the) dummy fibres so that they cross over the dummy fibre.
Another use to which couplers constructed in accordance with the present invention can be put is as N-channel demultiplexer/multiplexers. Figure 5 shows an embodiment of a 4-channel demultiplexer. Light at four different wavelengths, 1280, 1295, 1310 and 1325nm is input at port 100. The four wavelengths are separated and respectively output through ports 101,102,103 and 1014. The demultiplexer is made up of three coupling sections respectively indicated at 110,120 and 130. To provide the required demultiplexing function each of these individual coupler sections has to have the spectral response shown in Figure 6. The spectral response curves in this Figure have been given the same numbers as the coupler sections that they refer to.Thus in the embodiment shown in Figure 5 coupler 110 passes wavelengths of 1295 and 1325nm but couples 1280 and 1310nm.
Coupler 120 passes 1310 to output port 102 and couples 12cnm to output port 101, whilst coupler 130 couples 1325 to output port 104 and passes 1295nm to output port 103. This combined action of the three coupler sections separates the simultaneously input wavelengths into their four constituent parts. In the embodiment of Figure 5 four single mode fibres 111,112,113 and 114 and two dummy fibres 115 and 116 are used. The manner in which they are arranged is shown in Figure 7 The first taper in the array of fibres is made as previously described to fabricate coupler section 110. The two outputs of coupler section 110 are then crossed over the dummy fibres as is shown in Figure 7.Another taper is then fabricated with the two coupler sections so formed kept electromagnetically isolated by the presence of the two dummy fibres.
The method of ensuring that each of the coupler sections has the desired spectral response is as follows.
If light at a specific wavelength is launched down one of a pair of parallel monomode fibres which are subjected to stretching and heating so that the two fibres fuse to provide a coupler it will be found that the output from one of the fibres will vary between maxima and minima as the stretching operation is carried out. At the same time the output of the other fibre will vary in a converse manner. This variation after a certain degree of stretching settles into a relatively steady beat with a fixed period. Thus by carrying out the tapering process until this degree of stretching has occurred, monitoring the output of one of the fibres and stopping the tapering process once the output has reached a maxima for a specific wavelength, it can be assumed that the output of the parallel, fused fibre will be at a minima for that wavelength.It is this reciprocal performance between the outputs of the two coupled fibres which enables the first coupling section 112 to be fabricated with the desired spectral response.
The fabrication of coupler sections 120 and 130 employs a similar procedure but with the some additional factors to be take into account. Because the coupler section 110 has already been fabricated the subsequent sections 120 and 130 cannot be given the required spectral response by launching light down the input port leading to section 110. Because of this the fabrication of coupler sections 120 and 130 involves launching light down what will eventually be the output ports. As previously mentioned coupler section 120 is arranged to couple 1280nm and pass 1310nm. To achieve this light at 1280 is launched down that output namely output 103, which is intended to give 1310nm as its output. This is the output of fibre 112.
The intensity of the transmitted light at the output of fibre 111, that is the end 121 of fibre 111 remote from output port 101, is monitored during the tapering process.
As with coupler section 110 the tapering process is combined until the heat period of the light intensity oscillations has settled into a relatively fixed period.
The tapering process is stopped when the output of light at 1280nm from fibre end 121 is at a maximum. As previously explained this means that the coupler section 120 will now couple light at 1280nm to output 101 andthat the spectral responses shown in Figure 6 will ensure that light at 1310nm is passed to output port 102.
Exactly the same procedure is carried out with the other two ports 103, 1014. Thus duringfåbricati-on light at 1325 is launched into port 103 and monitored at 122 to produce a maxima at that port.
It is of course possible to carry out the converse operations with exactly the same results.
Namely, when fabricating section 120 light at 1310nm could be launched at output port 101 and the tapering process stopped when the monitored output at 121 is at a minimum. This again ensures that coupling section 120 will pass light at 1310nm to output port 102. The only remaining problem of fabrication is the fact that the coupler sections 120, 130 have to be "out-of-phase" by E period to satisfy the response curves in Figure 6.
As the two coupler sections are fabricated simultaneously this involves imparting a very slight differential stretch to the two different sections.
One way of achieving this is to tension the two sections by attaching the fibres to the circumference of separate wheels or pulleys which are driven in synchronism.
However, one of the wheels is given a slightly greater diameter than the other so that the amount of stretch imparted per degree of rotation varies between the two wheels. The difference in diameter can be discovered empirically.
It will now be apparent that whilst the device of Figure 5 has been described as a demultiplexer taking its input at 100, the device is capable of functioning equally well as a multiplexer with ports 101, 102, 103 and 104 acting as inputs for separate wavelengths to be multiplexed, and input port 100 becoming the output port.
The previous description has been directed to producing fibre optic couplers using monomode fibres using one or more dummy fibres. The present invention can, however, be utilised with multimode fibres and without the necessity of using dummy fibres.
Taking again the example of a 4x4 coupler and referring to Figure 8 of the drawings it can be seen that at A four fibres 100, not necessarily mono-mode, have been laid side-by-side with twists indicated at 101 and 102. Heat is applied around the area of the twists 101 and 102 and the four fibres stretched to make two parallel couplers separated by an air gap, the previous twists having now become coupling sections. During this operation light is launched down the fibres and monitored as already described in this specification.
The next step is shown at B in Figure 8. The inner two fibres are crossed-over at 103. The final step is shown at C where the outer pairs of fibres are twisted over at 104 and 105 to make two further couplings. The air gap between the couplers is taken up by a potting medium when the device is finally packaged. Couplers fabricated in this manner can be utilised in the applications already described in this specification. Figure 9 shows the final, but unpotted, 4x4 coupler, with the coupling section shown as in
Figure 8 at 101, 102, 104 and 105.
There is also a requirement for an optical sensor having the general configuration shown in Figure 10.
The essential nature and advantages of such a sensor are fully discussed in a paper by I.P. Giles, S. McNeil and
B. Culshaw in a paper entitled "A stable remote intensity based optical fibre sensor11 in the journal of the
Institute of Physics. However the main advantage is that the sensor'is immune to changing fibre losses so that it is only the effect of the probe located between ends 5 and 6 which affects the measurement. This probe can be of any suitable type and can be responsive to temperature pressure as any other measurement. The fibre network which is the basis of the sensor is very similar to that described with regard to Figures 8 and 9 except that parts 5 and 6 are not connected; The way that this is achieved can be appreciated from Figures 11 and 12.
An extra fibre is included and there are two cross-over points at 110 and 120. The coupling sections 111, 112, 113 and 114 correspond to the coupling sections of the 4x4 embodiment shown in Figure 9. Also present are low loss tapers 115 and 116 in the added fibre.
Figure 12 is a schematic view of the network shown in Figure 11.
Claims (8)
1. A method of fabricating an NxN optical coupler where N is at least equal to 4, the method being characterised in that it comprises the steps of locating two pairs of optical fibres side by side, applying simultaneous tension and heat to the fibres so as to generate a biconical taper in the fibres so located, and to cause the fibres of each pair to fuse together to form two couplers, displacing one fibre of each pair so that each displaced fibre lies in the position vacated by the other fibre, and generating a second biconical taper in the rearranged fibres so as to fabricate two further couplers.
2. A method as claimed in Claim 1, and characterised in that an air gap is maintained between the couplers so formed, and a potting compound is utilised to fill this air gap.
3. A method as claimed in Claim 1, and characterised in that each pair of fibres is separated by a dummy fibre.
4. A method as claimed in Claim 1 and characterised in that at least three pairs of fibres are provided, the fibres of each pair being coupled together, one fibre of each of the coupled pairs then being coupled with a fibre of another of the coupled pairs, and the process being repeated to provide an NxN coupler where N is greater than 4.
5. A method as claimed in Claim 3 and characterised in that at least three pairs of fibres are provided, the fibres of each pair being coupled together, one fibre of each of the coupled pairs then being coupled with a fibre of another of the coupled pairs, and the process being repeated to provide an NxN coupler where N is greater than 4.
6. An optical coupler characterised in that it is constructed in accordance with a method as claimed in any one of the preceding claims.
7. A method of fabricating an optical coupler substantially as hereinbefore described with reference to any one of the Figures 1 to 3 or Figure 8 of the accompanying drawings.
8. An optical device substantially as hereinbefore described with reference to any one of Figures 4, 5 or 10.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| GB8706678A GB2199418B (en) | 1986-03-24 | 1987-03-20 | Branching optical fibre coupler having biconical tapers. |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| GB868607286A GB8607286D0 (en) | 1986-03-24 | 1986-03-24 | Optical fibres |
| GB868616387A GB8616387D0 (en) | 1986-07-04 | 1986-07-04 | Compact fibre optic couplers |
| GB8706678A GB2199418B (en) | 1986-03-24 | 1987-03-20 | Branching optical fibre coupler having biconical tapers. |
Publications (3)
| Publication Number | Publication Date |
|---|---|
| GB8706678D0 GB8706678D0 (en) | 1987-04-23 |
| GB2199418A true GB2199418A (en) | 1988-07-06 |
| GB2199418B GB2199418B (en) | 1990-08-22 |
Family
ID=27262968
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| GB8706678A Expired - Fee Related GB2199418B (en) | 1986-03-24 | 1987-03-20 | Branching optical fibre coupler having biconical tapers. |
Country Status (1)
| Country | Link |
|---|---|
| GB (1) | GB2199418B (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5802224A (en) * | 1994-05-23 | 1998-09-01 | Kyocera Corporation | Optical coupler for performing light branching and light mixing/branch filtering in a light communication network |
| GB2377505A (en) * | 2001-07-10 | 2003-01-15 | Jds Uniphase Corp | Fused optic fibre couplers |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB1384567A (en) * | 1972-06-12 | 1975-02-19 | Soval Ltd | Fibre-optical viewing devices |
| EP0174014A2 (en) * | 1984-09-06 | 1986-03-12 | Hitachi, Ltd. | Optical star coupler and method for manufacturing the same |
-
1987
- 1987-03-20 GB GB8706678A patent/GB2199418B/en not_active Expired - Fee Related
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB1384567A (en) * | 1972-06-12 | 1975-02-19 | Soval Ltd | Fibre-optical viewing devices |
| EP0174014A2 (en) * | 1984-09-06 | 1986-03-12 | Hitachi, Ltd. | Optical star coupler and method for manufacturing the same |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5802224A (en) * | 1994-05-23 | 1998-09-01 | Kyocera Corporation | Optical coupler for performing light branching and light mixing/branch filtering in a light communication network |
| GB2377505A (en) * | 2001-07-10 | 2003-01-15 | Jds Uniphase Corp | Fused optic fibre couplers |
| US6839490B2 (en) | 2001-07-10 | 2005-01-04 | Jds Uniphase Corporation | Method of making sequential coupler arrangements and resulting devices |
Also Published As
| Publication number | Publication date |
|---|---|
| GB8706678D0 (en) | 1987-04-23 |
| GB2199418B (en) | 1990-08-22 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| PCNP | Patent ceased through non-payment of renewal fee |